/*===================================================================*/ /* NRDF D1834 Data No.1 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,1; D#=D1834; TITLE=/M1 and Gamow-Teller transitions in T=1/2 nuclei 23Na and 23Mg/; PURPOSE=/To compare analogous M1 and Gamow-Teller transitions in the pair of mirror nuclei 23Na and 23Mg/; ATH=(Y.FUJITA'1', Y.SHIMBARA'1', I.HAMAMOTO'2', T.ADACHI'1', G.P.A.BERG'3', H.FUJIMURA'3', H.FUJITA'1', J.GORRES'4', K.HARA'3', K.HATANAKA'3', J.KAMIYA'3', T.KAWABATA'3', Y.KITAMURA'3', Y.SHIMIZU'3', M.UCHIDA'5', H.P.YOSHIDA'3', M.YOSHIFUKU'1', M.YOSOI'5'); INST-ATH=(2JPNOSA'1', 2SWDLND'2', 2JPNRCN'3', 1USANOT'4', 2JPNKTO'5'); /* '1' Department of Physics */ /* '2' Division of Mathematical Physics */ /* '4' Department of Physics */ /* '5' Department of Physics */ REF=PR/C; VLP=66(2002)044313; RCTS=23NA(3HE,T)23MG; PHQS=TRNSN-STRGTH'6'; /* '6' The GT transition strength (B(GT)) */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,1; RTY=RRG-RCT'7'; /* '7' Charge Exchange reaction */ PHQ=TRNSN-STRGTH'8'; /* '8' The GT transition strength (B(GT)) */ ENR=X%'9'; /* '9' The target is effectively a mixture of 23Na, carbon isotopes 12C and 13C (naturalabundance 98.9% and 1.1%, respectively), and oxygen isotopes 16O and 18O (natural abundance 99.8% and 0.2%, respectively). */ CHM=X'10'; /* '10' Na2CO3 */ PHYS-FORM=SLD; THK-TGT=[2MG/CM**2; BAC=X'11'; /* '11' polyvinyl alcohol [Y. Shimbara et al., Nucl. Instrum. Meth. Phys. Res. A (to be published)] */ POL-TGT=0%; ALGN-TGT=0%; ACC=CYC'12'; /* '12' K=400, RCNP Ring Cyclotron */ INST-ACC=2JPNRCN; INC-ENGY-LAB=140MEV/A; POL-PRJ=0%; DET-PARTCL=T; COINC=NO; ANT-COINC=NO; DET-SYS=(MAG'13',MWDC'14'); /* '13' Grand Raiden spectrometer [M.Fujiwara et al., Nucl. Instrum. Method phys. Res. A 422 (1999) 484]. Outgoing tritons within the full acceptance of the spectrometer [ +-20 mrad and +-40 mrad in horizontal (x) and vertical (y) directions, respectively] were momentum analyzed. */ /* '14' Outgoing tritons were detected at the focal plane with a multiwire drift-chamber system allowing track reconstruction [T. Noro et al., RCNP, Annual Report 1991, p.177]. */ ERS-DET=45KEV'15'; /* '15' full width at half maximum */ CALB-DET=/ Known states of 13N and 16F, which were observed in the spectrum of Mylar target, and the 26Al states, which were observed in the 26Mg(3He,t)26Al spectrum taken under the same condition as for the Na2CO3 target, were used as calibration standard. /; /* Analysis: - The B(GT) values were calculated by using the proportionality (Eq.32) from their peak intensities after excitation-energy correction was made. RCT=23NA(3HE,T)23MG; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,1; INC-ENGY-LAB=140MEV/A; RSD=23MG; THTL=0DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; EXC-ENGY DELTA-EXC-ENGY TRNSN-STRGTH'16' DELTA-TRNSN-STRGTH'16' FLAG'17' (MEV) (MEV) (NODIM) (NODIM) (NODIM) 0.0 +-X 0.340 +-0.014 1. 0.451 +-X 0.146 +-0.006 2. 2.360 +-0.003 0.055 +-0.004 X 2.906 +-0.003 0.193 +-0.011 X 3.860 +-0.003 0.055 +-0.004 X 4.357 +-0.003 0.250 +-0.013 X 5.291 +-0.003 0.066 +-0.005 X 5.658 +-0.004 0.270 +-0.017 X 5.712 +-0.008 0.061 +-0.009 X 6.550 +-0.003 0.116 +-0.007 X 6.818 +-0.003 0.028 +-0.003 X 6.911 +-0.003 0.057 +-0.004 X 8.168 +-0.004 0.290 +-0.015 X 8.452 +-0.005 0.039 +-0.003 X 9.159 +-0.006 0.069 +-0.005 X 9.159 +-0.006 0.069 +-0.005 X 10.290 +-0.007 0.046 +-0.004 X 11.132 +-0.008 0.062 +-0.005 X \END; /*===================================================================*/ |